Problem 90
Question
Power meters enable cyclists to obtain power measurements nearly continuously. The meters also calculate the average power generated over a time interval. Professional riders can generate 6.6 watts per kilogram of body weight for extended periods of time. Some meters calculate a normalized power measurement to adjust for the physiological effort required when the power output changes frequently. Let the random variable \(X\) denote the power output at a measurement time and assume that \(X\) has a lognormal distribution with parameters \(\theta=5.2933\) and \(\omega^{2}=0.00995 .\) The normalized power is computed as the fourth root of the mean of \(Y=X^{4}\). Determine the following: (a) Mean and standard deviation of \(X\) (b) \(f_{Y}(y)\) (c) Mean and variance of \(Y\) (d) Fourth root of the mean of \(Y\) (e) Compare \(\left[E\left(X^{4}\right)\right]^{1 / 4}\) to \(E(X)\) and comment.
Step-by-Step Solution
VerifiedKey Concepts
Power output analysis
A cyclist's power output, modeled by a random variable, is often assumed to have a lognormal distribution. This is because even minor changes in power can impact an athlete's performance significantly, reflecting a more skewed nature of data. The data skewness towards higher power outputs makes the lognormal distribution a suitable choice for analysis because it can describe data that is positively skewed. This understanding of power output data is crucial as it influences training programs and race strategies.
Mean and standard deviation calculation
- \(E(X) = e^{\theta + \frac{\omega^2}{2}}\)
The standard deviation \(\sigma_X\) provides insight into the variability of the power output:
- \(\sigma_X = e^{\theta + \frac{\omega^2}{2}}\sqrt{e^{\omega^2} - 1}\)
Probability density function derivation
- The new mean parameter \(\mu_Y = 4\theta\)
- The variance parameter \(\sigma_Y^2 = 4^2 \cdot \omega^2\)
Variance calculation
- \(Var(Y) = (e^{8 \cdot \omega^2} - 1)e^{2(4\theta + 8 \cdot \omega^2)}\)